首页|正弦波纹微通道内单相流动及换热特性数值研究

正弦波纹微通道内单相流动及换热特性数值研究

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为了分析正弦波纹微通道中的单向流动和对流换热特性,通过数值模拟研究了波幅为 125~500 μm范围的正弦波纹微通道中,入口雷诺数Re在100~1 000 条件下冷却液的流动和换热特性.研究结果表明:波幅和雷诺数的增加均会导致流动压降和摩擦因子增加.当Re=400、波幅A从125 μm增加至500 μm时,流动压降和摩擦因子分别升高至原始值的3 倍和2 倍,从而显著增加了流动阻力,表明波幅增强了流道内部的流动和扰动,提高了换热效率;当波幅A=500 μm、雷诺数Re由100 增加至1 000 时,压降增大约50 倍,摩擦因子增大约10 倍,传热系数增大5 倍,表明随着雷诺数的增加,流道内冷却剂的流速和摩擦因子也随之增加,流动扰动性越强,传热系数也越高.
Numerical Study on Single-phase Flow and Heat Transfer Characteristics in Sinusoidal Wavy Microchannels
In order to analyze the single-phase flow and convective heat transfer characteristics in sinu-soidal wavy microchannels,numerical simulations were conducted to investigate the fluid flow and heat transfer characteristics of the coolant in sinusoidal wavy microchannels with wave amplitudes ranging from 125 to 500 μm,under inlet Reynolds numbers of 100 to 1 000.The research results indicate that an in-crease of wave amplitude and Reynolds number leads to an increase of flow pressure drop and friction fac-tor.Under the conditions of inlet Reynolds number Re of 400 and wave amplitude A from 125 to 500 μm,the flow pressure drop and friction factor increase to 3 and 2 times of the original values,re-spectively,significantly increasing the flow resistance.The larger wave amplitude enhances the flow and disturbance inside the flow channel,improving heat transfer efficiency;when the wave amplitude is 500 μm and Reynolds number increases from 100 to 1 000,the pressure drop,friction factor and the heat transfer coefficient increase by 50,10 and 5 times respectively.With the increase of Reynolds number,the flow velocity and friction factor of the coolant in the flow channel also increase.The stronger the flow disturbance,the higher the heat transfer coefficient.

wavy microchanneltemperature uniformityenhanced heat transferflow resistancenu-merical calculation

李辉、吴明昊、谷晓建、王祥和

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中国船舶集团有限公司第七○三研究所,黑龙江 哈尔滨 150078

中国人民解放军91526 部队,广东 湛江 524000

波纹微通道 温度均匀性 强化换热 流动阻力 数值计算

2024

热能动力工程
中国 哈尔滨 第七0三研究所

热能动力工程

CSTPCD北大核心
影响因子:0.345
ISSN:1001-2060
年,卷(期):2024.39(5)